共查询到20条相似文献,搜索用时 15 毫秒
1.
J. Jimenez-Vicente E. Battaner C. Porcel M. Rozas H. Castañeda 《Astrophysics and Space Science》2001,276(2-4):445-449
We have studied the kinematics of the ionized gas in the nearly face-on galaxy NGC 3938 by means of observations made with
theFabry–Perot interferometer TAURUS II at the William Herschel Telescope, using the Hα line. We have been able to produce high-resolution velocity and velocity-dispersion maps which allow us to make a detailed
study of the kinematics of the ionized gas. In particular we have found that the vertical velocity dispersion is constant
with galactocentric radius, as has already been found for the atomic and molecular gas in this galaxy. This suggests the existence
of several heating mechanisms in the disc acting simultaneously to produce the observed behaviour.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
2.
S. A. Hakopian S. K. Balayan S. N. Dodonov A. V. Moiseev A. A. Smirnova 《Astrophysics》2012,55(1):1-13
The methods of panoramic (3D) spectroscopy are used by us in a detailed study of galaxies with ongoing star formation chosen
from among objects in seven selected fields of the Second Byurakan Survey (SBS). This article deals with the irregular galaxy
SBS 1202 + 583, which our classification scheme identifies as being in a continuous phase of star formation. Observations
were made with the panoramic spectrographs MPFS at the 6-m telescope of the Special Astrophysical Observatory (SAO) of the
Russian Academy of Sciences and VAGR at the 2.6-m telescope of the Byurakan Astrophysical Observatory (BAO) in Armenia. The
data are used to construct maps of the radiative fluxes in the continuum and various emission lines. Special attention is
devoted to analyzing the emission in the Hα hydrogen recombination line and in the forbidden low-ionization doublets of nitrogen [NII] λλ6548, 6583 and sulfur [SII] λλ6716, 6731, and the ratios of the intensities of the forbidden lines to Hα. The observable characteristics (size, Hα fluxes, etc.) of nine HII regions are studied. The estimated current rates of star formation in the individual HII regions
based on the Hα fluxes lie within the range of 0.3-1.2⨀ M /year. The dependence of the ratio of the intensities of the emission in these above mentioned forbidden doublets on the
rate of star formation in the HII regions is found. 相似文献
3.
Optical CCD imaging with Hα and [SII] filters and spectroscopic observations of the galactic supernova remnant G85.9-0.6 have been performed for the
first time. The CCD image data are taken with the 1.5 m Russian-Turkish Telescope (RTT150) at TüBİTAK National Observatory
(TUG) and spectral data are taken with the Bok 2.3 m telescope on Kitt Peak, AZ.
The images are taken with narrow-band interference filters Hα, [SII] and their continuum. [SII]/Hα ratio image is performed. The ratio obtained from [SII]/Hα is found to be ∼0.42, indicating that the remnant interacts with HII regions. G85.9-0.6 shows diffuse-shell morphology. [SII]λ
λ6716/6731 average flux ratio is calculated from the spectra, and the electron density N
e
is obtained to be 395 cm−3. From [OIII]/Hβ ratio, shock velocity has been estimated, pre-shock density of n
c
=14 cm−3, explosion energy of E=9.2×1050 ergs, interstellar extinction of E(B−V)=0.28, and neutral hydrogen column density of N(HI)=1.53×1021 cm−2 are reported. 相似文献
4.
Results from a spectrophotometric study of the galaxy Kaz 701 are presented. Spectra of this galaxy were obtained on the 2.6-m
telescope at the Byurakan Observatory with the SCORPIO spectral camera. In the spectra of Kaz 701, strong Hα, [OIII] λλ5007,
4959, and Hβ emission were observed, and the [SII]λλ6731, 6717 lines were observed with moderate intensities, while the [NII]λ6584
line was scarcely noticeable in the spectra obtained in 2004, but was much more intense in the spectra of 2009. The lines
observed in the spectrum of this galaxy are typical of type Sy2 galaxies. A component was observed in the red wings of both
the Hα and Hβ lines in the data of 2004, but, although these lines were stronger, these components were absent in the spectra
taken in 2009. The relative intensities, equivalent widths, and half widths of these lines are given. These data, obtained
in different observation periods (2004 and 2009), differ greatly; that is, the emission is variable. 相似文献
5.
The galaxy NGC6384 has been observed with an IPCS through Hα and [NII] narrow-band interference filters for direct imagery with the 2.6-m Byurakan telescope. We studied the main physical
parameters of the identified 98 HII regions, their diameter and luminosity functions, as well the [NII]/Hα ratio distribution. The integrated distribution function of the HII region diameters can be well fitted by the exponential
function. The characteristic diameter has the value (Do = 217 pc) predicted for a galaxy of its measured luminosity. The luminosity
function of HII regions has a double power law profile with relatively shallow slope at low luminosities (α = −0.4), an abrupt
turnover at logL(Hα) ≈ 38.75, and sharper slope at higher luminosities (α = −2.3). The correlation between the luminosity and diameter of HII
regions confirms that in general they are constant density, radiation-bound systems. [NII]/Hα ratio data for the HII regions show that there is a negative radial gradient of [NII]/Hα. In the central region of the galaxy, nitrogen abundance is higher than in the periphery. The properties of the HII region
population of this AGN galaxy do not differ significantly from the properties of the HII region population of the “normal”
galaxies. Reexamining the location of the type Ia SN 1971L in the galaxy, we confirm that it lies on the spiral arm at about
8″.6 far from the closest HII region N 53 (F81). Such a location can be taken as proof that the progenitor of this SN does
not belong to an old, evolved stellar population.
Published in Astrofizika, Vol. 50, No. 4, pp. 519–533 (November 2007). 相似文献
6.
The results of morphological and spectral study of the galaxies Kaz 5, Kaz 92, and Kaz 390 are presented. The observations
were made on the 2.6-m telescope at the Byurakan Observatory with the VAGR microlenses spectrograph. Isophotes of the images
of the galaxies are constructed in the Hα, [NII] λλ6584 , 6548, and [SII] λλ6731, 6717 emission lines and in the continuum. The masses of Kaz 5 and Kaz 92 are determined to be 8.6 × 108 M⊙ and 6.1 × 109 M⊙ , respectively. The mass of the gaseous component in the centers of regions I and IV of Kaz 390, which encompass a 1 pixel
area, are also determined. The morphological structure of the central region of Kaz 5 in the observed spectral range, λλ6400–6800?, differs completely from the structure of the same part of the galaxy observed with the 6-m and 2.5-m telescopes. It is shown
that these differences in the structure in images of Kaz 5 are mostly explained by the comparatively low resolution of the
telescope in combination with the VAGR spectrograph. Absorbing matter also contributes to this effect. It is also shown that
a “deficit” of nitrogen has been observed in the region of Kaz 390 studied here (a circle of diameter 40″).
Translated from Astrofizika, Vol. 52, No. 1, pp. 63–74 (February 2009). 相似文献
7.
L. Tomas-Calderon J.A. Acosta-Pulido B. Vila-Vilaro I. Perez-Fournon 《Astrophysics and Space Science》1998,263(1-4):123-126
We present preliminary results of long-slit spectroscopic observations of the extended emission line region (hereafter, EELR)
in NGC 4388. We detect broad emission lines in the line complexes Hα+[NII] and [SII] which can be modelled by the superposition
of several narrow components. Multicomponent line profiles appear at positions very close to the ionization cone axis. There
is also some correspondence with the radio emission, which suggests that there is interaction between the radio jets and the
ionized gas. We do not confirm the claim of a broad Hα component (FWZI=4000 km/s) by Shields and Filippenko (1996).
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
8.
We report the results of a survey of the H i environment of NGC 6946 in a search for gas-rich companions to the galaxy. Such gas-rich companions could include material left over from the galaxy assembly process which could persist into the current day around an isolated galaxy such as NGC 6946. NGC 6946 is prolifically forming stars, has a nuclear starburst, and has widespread high-velocity clouds associated with the disc. All of these features could be explained by the accretion of low-mass H i clouds by NGC 6946. Our survey recovered two previously detected dwarf galaxies associated with NGC 6946, but otherwise found no signatures of interactions in the NGC 6946 system. The companions are small enough, and distant enough from NGC 6946 that they should have minimal effect on the main galaxy. Some tidal debris may be expected due to interaction between the two dwarf galaxies, but none is observed. This could be because it is at low column densities, or because the dwarf galaxies are more separated than they appear on the sky. This study of the system suggests that NGC 6946 is a gravitationally bound system with two dwarf galaxies in stable orbits about the larger primary galaxy. 相似文献
9.
The peculiar galaxy NGC 4650 A (α=12h 42m. 1; = δ—40° 26′; 1950·0) has been studied by means of direct and spectral observations with the ESO 3·6-m telescope. It is
interpreted as a prolate, elliptical galaxy surrounded by a warped ring of H II regions, dust and stars. The distance is 47
Mpc (H
0=55 km s−1 Mpc−1). The ring is seen nearly edge-on (inclination 85°) and it rotates. It has a diameter of about 21 kpc and is bluer than the
elliptical galaxy for which the (M/L
v) ratio is ∼12 in solar units. The observed configuration may be the result of interaction with the nearby galaxy, NGC 4650. 相似文献
10.
We analyze the emission component of galaxy nuclei at very low intensity levels (W(H)2Å). This emission level is considerably lower than that of classical LINERS like NGC 1052. We have access to weaker emission lines by averaging spectra with similar line ratios for H [NII], and [SII]. From the resulting spectrum for very low level emission nuclei, the [SII] 6717, 6731/[SIII] 9069, 9532 line ratio criterion (Diazet al., 1985a) unambiguously shows that shock-wave heating is the mechanism responsible for the ionization in such objects. 相似文献
11.
Observations of the H272α recombination line towards the galactic centre show features near VLSR= 0, −50 and + 36 kms−1. We have combined the parameters of these features with the available H166α measurements to obtain the properties of the
ionized gas present along the line of sight and also in the ‘3 kpc arm’. For the line-of-sight ionized gas we get an electron
density around 7 cm−3 and a pathlength through it ∼ 10–60 pc. The emission measure and the electron temperature are in the range 500–2900 pc cm−6 and 2000–6000 K. respectively. The ionized gas in the 3 kpc arm has an electron density of 30 cm−3 and extends over 9 pc along the line of sight if we assume an electron temperature of 104 K. Using the available upper limit to the intensity of the H351α recombination line, we show that the distributed ionized
gas responsible for the dispersion of pulsar signals should have a temperature >4500 K. and a minimum filling factor of 20
per cent. We also show that recombination lines from the ‘warm ionized’ gas proposed by McKee & Ostriker (1977) should be
detectable in the frequency range 100–150 MHz towards the galactic centre with the sensitivity available at present. 相似文献
12.
We use the catalogue of HII regions obtained from a high quality continuum-subtracted Hα image of the grand-design spiral galaxy NGC 7479, to construct the luminosity function (LF) for the HII regions(over 1000)
of the whole galaxy. Although its slope is within the published range for spirals of the same morphological type, the unusually
strong star formation along the intense bar of NGC 7479 prompted us to analyse separately the HII regions in the bar and in
the disc. We have calculated the physical properties of a group of HII regions in the bar and in the disc selected for their
regular shapes and absence of blending. We have obtained galaxy-wide relations for the HII region set: diameter distribution
function and also the global Hα surface density distribution. As found previously for late-type spirals, the disc LF shows clear double-linear behaviour
with a break at log L
∼ 38.6 (in erg -1). The bar LF is less regular. This reflects a physical difference between the bar and the disc in the properties of their
populations of regions.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
13.
This is a study of optical emission lines of the nucleus of the Seyfert galaxy NGC 3227. This work is based on 53 spectrograms
obtained with the 6-m telescope at the brightness maximum of this galactic nucleus on January 12–15, 1977. A set of profiles
of the hydrogen Hα, and Hβ lines and the equivalent widths (EWλ) of six emission lines and blends averaged over series of observations are presented. Broadening of the hydrogen line profiles
was observed over the three days. At a level of 0.50 times the peak brightness the hydrogen line profiles were broadened by
12%, 35%, and 44%, respectively. The broadening of the Hβ line was accompanied by a reduction in its equivalent width (EW
;
). It is suggested that a flare was observed in the nucleus of the galaxy on a time scale of 3 days, possibly caused to a
shock wave in long-lived flows from the galaxy nucleus.
__________
Translated from Astrofizika, Vol. 49, No. 4, pp. 499–510 (November 2006). 相似文献
14.
The velocity field in the galaxy Mark 8 is studied by means of observations with the 2.6-m telescope at the Byurakan Astrophysical
Observatory using the VAGR spectrograph. In the optical range, the central portion of this galaxy consists of five bright
condensations which are superassociations (SA). These studies were made in a wavelength range that encompasses images of the
galaxy in the Hα and [NII] λλ6548 and 6583Å emission lines. The radial velocity field was obtained. The velocities of all
the superassociations were measured and a rotation curve constructed for the galaxy. The relative intensities of the emission
lines have been determined. Images are constructed in the Hα and [NII] lines and in the red continuum. It is concluded that
the superassociations were formed together and are, as a whole, young. The shape of the rotation curve shows that Mark 8 is
an isolated galaxy with a composite multicomponent nucleus.
Translated from Astrofizika, Vol. 51, No. 4, pp. 543–553 (November 2008). 相似文献
15.
H.B. Ann 《Astrophysics and Space Science》2001,276(2-4):683-690
We have conducted UBVRI and Hα CCD photometry of five barred galaxies (NGC 2523, NGC 2950, NGC 3412, NGC 3945 and NGC 5383),along with SPH simulations,
in order to understand the origin of young stellar populations in the nuclei of barred galaxies. The Hα emission, which is thought to be emitted by young stellar populations, is either absent or strongly concentrated in the nuclei
of early-type galaxies (NGC 2950, NGC 3412 and NGC 3945),while they are observed in the nuclei and circumnuclear regions of
intermediate-type galaxies with strong bars (NGC 2523 and NGC 5383).SPH simulations of realistic mass models for these galaxies
show that some disc material can be driven into the nuclear region by a strong bar potential. This implies that the young
stellar populations in the circumnuclear regions of barred galaxies can be formed out of such gas. The existence of nuclear
dust lanes is an indication of an ongoing gas inflow and extremely young stellar populations in these galaxies, because nuclear
dust lanes such as those in NGC 5383 are not long-lasting features according to our simulations.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
16.
Observations on the 6-m telescope in the Hα line and in the continuum are reported for 10 dwarf companions of the galaxy M31:
And I, And II, And III, And V, And IX, And X, Cass dSph, Peg DSph, NGC147, NGC221, and one irregular dwarf galaxy in the background,
And IV. All the observed companions of M31 have current star formation rates (SFR) on the order of or less than 10−6 M⊙ /yr. On a “star formation rate-neutral hydrogen mass” diagram for galaxies in the local volume, the dwarf spheroidal companions
of Andromeda lie in the region of extremely low values for these parameters.
__________
Translated from Astrofizika, Vol. 49, No. 3, pp. 337–350 (August 2006). 相似文献
17.
Curtis Struck Daniel C. Smith 《Monthly notices of the Royal Astronomical Society》2009,398(3):1069-1081
The existence of partially ionized, diffuse gas and dust clouds at kiloparsec scale distances above the central planes of edge-on, galaxy discs was an unexpected discovery about 20 years ago. Subsequent observations showed that this extended or extraplanar diffuse interstellar gas (EDIG) has rotation velocities approximately 10–20 per cent lower than those in the central plane, and has been hard to account for. Here, we present results of hydrodynamic models, with radiative cooling and heating from star formation. We find that in models with star formation generated stochastically across the disc, an extraplanar gas layer is generated as long as the star formation is sufficiently strong. However, this gas rotates at nearly the same speed as the midplane gas. We then studied a range of models with imposed spiral or bar waves in the disc. EDIG layers were also generated in these models, but primarily over the wave regions, not over the entire disc. Because of this partial coverage, the EDIG clouds move radially, as well as vertically, with the result that observed kinematic anomalies are reproduced. The implication is that the kinematic anomalies are the result of three-dimensional motions when the cylindrical symmetry of the disc is broken. Thus, the kinematic anomalies are the result of bars or strong waves, and more face-on galaxies with such waves should have an asymmetric EDIG component. The models also indicate that the EDIG can contain a significant fraction of cool gas, and that some star formation can be triggered at considerable heights above the disc mid-plane. We expect all of these effects to be more prominent in young, forming discs, to play a role in rapidly smoothing disc asymmetries and in working to self-regulate disc structure. 相似文献
18.
P. Amram C. Mendes de Oliveira H. Plana C. Balkowski M. Bolte 《Astrophysics and Space Science》2002,281(1-2):397-400
We present kinematics and photometric evidence for the presence of seven candidate tidal dwarf galaxies in Stephan's Quintet.
The central regions of the two most probable parent galaxies, NGC 7319 and NGC 7318B, contain little or no gas whereas the
intragroup medium and, in particular, the optical tails that seem to be associated with NGC 7318B are rich in cold and ionized
gas. Two tidal dwarf candidates may be located at the edge of a tidal tail, another located within a tail, and for the four
others there is no obvious stellar/gaseous bridge between them and the parent galaxy. Two of the candidates are associated
with H I clouds, one of which is, in addition, associated with a CO cloud. All seven regions have low continuum fluxes and
high Hα luminosity densities [F(Hα) = (1-60) × 10-14 ergs s-1 cm-2]. Their magnitudes (MB = –16.1 to –12.6), sizes (∼ 3.5 h75
-1 kpc), colors (typically B – R = 0.7), and gas velocity gradients (∼ 8 –26 h75 km s-1 kpc-1) are typical for tidal dwarf galaxies. In addition, the ratios between their star formation rates determined from Hα and
from the B-band luminosity are typical of other tidal dwarf galaxies. The masses of the tidal dwarf galaxies in Stephan's
Quintet range from ∼ 2 × 108 to 1010 M⊙, and the median value for their inferred mass-to-light ratios is 7 (M/L)⊙. At least two of the systems may survive possible ‘fallbacks’ or disruption by the parent galaxies and may already be, or
turn into, self-gravitating dwarf galaxies, new members of the group.
This revised version was published online in September 2006 with corrections to the Cover Date. 相似文献
19.
Using the method of two-dimensional spectroscopy, we have investigated the kinematics and distribution of the gas and stars
at the center of the early-type spiral galaxy NGC 7177 with a mediumscale bar as well as the change in the mean age of the
stellar population along the radius. A classical picture of radial gas inflow to the galactic center along the shock fronts
delineated by dust concentration at the leading edges of the bar has been revealed. The gas inflow is observed down to a radius
R = 1″.5−2″, where the gas flows at the inner Lindblad resonance concentrate in an azimuthally highly inhomogeneous nuclear
star formation ring. The bar in NGC 7177 is shown to be thick in z coordinate—basically, it has already turned into a pseudo-bulge as a result of secular dynamical evolution. The mean stellar
age inside the star formation ring, in the galactic nucleus, is old, ∼10 Gyr.Outside, at a distance R = 6″−8″ from the nucleus, the mean age of the stellar population is ∼2 Gyr. If we agree that the bar in NGC 7177 is old,
then, obviously, the star formation ring has migrated radially inward in the last 1–2 Gyr, in accordance with the predictions
of some dynamical models. 相似文献
20.
Maite Rozas Almudena Zurita John E. Beckmann/snm> 《Astrophysics and Space Science》2001,276(2-4):1179-1188
We combine Hα and broad-band optical imaging and Hα velocity mapping over the face of the barred galaxy NGC 3359, obtained within the BARS programme on the Canary Island telescopes
(Lourenso and Beckman, these proceedings).From the Hα image we have determined the positions, fluxes and diameters of a total of 547 HII regions, and computed their luminosity
function whose slope is within the range of those of morphologically similar galaxies found in the literature. We have gone
on to quantify other statistical properties, such as the diameter distribution and the flux densities of the regions. Using
Fabry-Perot mapping in Hα with the TAURUS II instrument, we have produced maps of velocity and velocity dispersion, and computed the rotation curve
out to ∼ 3 scale lengths from the centre of the galaxy. From the map of the residual velocities we detected streaming motions
in the gas across the spiral arms and the presence of non-circular motions of order 30–40 km s-1 around the bar: the gas response to the gravitational potential.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献